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Authors: Leila C. Powell, Scott T. Kay and Arif Babul. Substructure in 2D X-ray images and weak lensing mass maps of galaxy clusters: A simulation study. Summary.
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Authors: Leila C. Powell, Scott T. Kay and Arif Babul Substructure in 2D X-ray images and weak lensing mass maps of galaxy clusters: A simulation study
Summary • Make 2D mass maps and X-ray surface brightness maps from cluster simulation to mimic perfect observations • Give statistics on mass substructure and X-ray substructure in 2D • Explore the relation among 2D mass, X-ray SB and 3D subhalo, to give insights into the gas stripping process and interpretations for observational data
Outline • Motivation & Background • Simulation & Data preparation(Map making and substructure detection) • 2D mass map: Completeness and Purity • 2D X-ray map • Discussion (Selection effect, Case study, gas physics, noise-adding) • Conclusion
Motivation & Background • Much Observational Study • X-ray: hot gas (T~1keV) emission • Weak lensing: DM mass • Do not necessarily trace each other: gas stripping • Tidal stripping • Ram pressure • Simulation: • DM subhalo (well-studied) • Gas substructure (not much systematic statistics, and mainly DM-bound gas) • Aim • Provide insight into the link between lensing map and X-ray map through underlying DM distribution • One way to give statistics on gas stripping, through the matching or mismatching of maps • Give predictions/expectations for future observations
Motivation & Background • Much Observational Study • X-ray: hot gas (T~1keV) emission • Weak lensing: DM mass • Do not necessarily trace each other: gas stripping • Tidal stripping • Ram pressure • Simulation: • DM subhalo (well-studied) • Gas substructure (not much systematic statistics, and mainly DM-bound gas) • Aim • Provide insight into the link between lensing map and X-ray map through underlying DM distribution • One way to give statistics on gas stripping, through the matching or mismatching of maps • Give predictions/expectations for future observations
Simulation & Data Preparation • Resimulations using GADGET2, standard cosmology • mp(DM)=4.3x10^8 (Msun/h), softening 10 kpc/h (z<1: 5kpc/h) • L~500Mpc/h • z=49~0, 50 outputs • adiabatic • three clusters, ~10^14Msun each, different MAHs • Fof group, R500, SUBFIND subhalo(DM+Gas)
Simulation & Data Preparation • Map making • z=0~1 • Cuboid projection(V=2R500X2R500X8R500),400x400 pixels (pixel size ~ softening) • Re-centered at brightest X-ray pixel
Simulation & Data Preparation • Detection technique • PSF smoothing to get observation • Background making: convolution with a broad filter • Background subtraction • Significance rejectionand FoF group-finding
Simulation & Data Preparation • Properties of 2D map
2D mass Map vs. 3D sub • Completeness and Obscuration (best: 3sigma)
2D mass Map vs. 3D sub • Purity (3sigma case)
2D mass vs. X-ray • A large fraction unmatched
Discussion: Selection effect • halo dynamical state (characterized by RMS centroid shift)
Discussion: Case Study • Case I: Partial stripping
Discussion: Case Study • Case II: Detachment • Dependent on numerical techniques (e.g, KHI)
Discussion: Case Study • Case III: missing mass-sub
Discussion: Case Study • Case IV: shared X-ray peak during merger
Discussion: Effect of Cooling • Cooling turned on till z~5, ~10% of gas had formed stars
Discussion: Effect of Cooling • Matching success with cooling
Conclusion • Completeness and purity of mass observations • The constructed 2D mass catalogue is 90% complete down to DM mass of 10^13Msun/h ( current weak lensing obs. limit) • Purity threshold of A>10^-3 (Mpc/h)^2, can be applied to other simulated maps • Scaling relation, can be used for mass estimation
Conclusion • A large fraction of substructures unmatched between 2D mass and X-ray, due to detachment or stripping • Dynamical state of clusters plays a role in the fraction of matching success • Inclusion of high-z cooling has only mild impact on the results • Future observations would detect more unmatched substrutures when noise is reduced and resolution enhanced